First application of the Oslo method in inverse kinematics
Abstract The %$\gamma %$-ray strength function (%$\gamma %$SF) and nuclear level density (NLD) have been extracted for the first time from inverse kinematic reactions with the Oslo method. This novel technique allows measurements of these properties across a wide range of previously inaccessible nuc...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Ingeberg, V. W. [verfasserIn] Siem, S. [verfasserIn] Wiedeking, M. [verfasserIn] Sieja, K. [verfasserIn] Bleuel, D. L. [verfasserIn] Brits, C. P. [verfasserIn] Bucher, T. D. [verfasserIn] Dinoko, T. S. [verfasserIn] Easton, J. L. [verfasserIn] Görgen, A. [verfasserIn] Guttormsen, M. [verfasserIn] Jones, P. [verfasserIn] Kheswa, B. V. [verfasserIn] Khumalo, N. A. [verfasserIn] Larsen, A. C. [verfasserIn] Lawrie, E. A. [verfasserIn] Lawrie, J. J. [verfasserIn] Majola, S. N. T. [verfasserIn] Malatji, K. L. [verfasserIn] Makhathini, L. [verfasserIn] Maqabuka, B. [verfasserIn] Negi, D. [verfasserIn] Noncolela, S. P. [verfasserIn] Papka, P. [verfasserIn] Sahin, E. [verfasserIn] Schwengner, R. [verfasserIn] Tveten, G. M. [verfasserIn] Zeiser, F. [verfasserIn] Zikhali, B. R. [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2020 |
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| Übergeordnetes Werk: |
Enthalten in: The European physical journal - Berlin : Springer, 1998, 56(2020), 2 vom: 20. Feb. |
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| Übergeordnetes Werk: |
volume:56 ; year:2020 ; number:2 ; day:20 ; month:02 |
| Links: |
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| DOI / URN: |
10.1140/epja/s10050-020-00070-7 |
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| Katalog-ID: |
SPR008300747 |
|---|
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| 100 | 1 | |a Ingeberg, V. W. |e verfasserin |4 aut | |
| 245 | 1 | 0 | |a First application of the Oslo method in inverse kinematics |
| 264 | 1 | |c 2020 | |
| 336 | |a Text |b txt |2 rdacontent | ||
| 337 | |a Computermedien |b c |2 rdamedia | ||
| 338 | |a Online-Ressource |b cr |2 rdacarrier | ||
| 520 | |a Abstract The %$\gamma %$-ray strength function (%$\gamma %$SF) and nuclear level density (NLD) have been extracted for the first time from inverse kinematic reactions with the Oslo method. This novel technique allows measurements of these properties across a wide range of previously inaccessible nuclei. Proton–%$\gamma %$ coincidence events from the %$\mathrm {d}(^{86}\mathrm {Kr}, \mathrm {p}\gamma )^{87}\mathrm {Kr}%$ reaction were measured at iThemba LABS and the %$\gamma %$SF and NLD in %$^{87}\mathrm {Kr}%$ was obtained. The low-energy region of the %$\gamma %$SF is compared to shell-model calculations, which suggest this region to be dominated by M1 strength. The %$\gamma %$SF and NLD are used as input parameters to Hauser–Feshbach calculations to constrain %$(\mathrm {n},\gamma )%$ cross sections of nuclei using the TALYS reaction code. These results are compared to %$^{86}\mathrm {Kr}(n,\gamma )%$ data from direct measurements. | ||
| 700 | 1 | |a Siem, S. |e verfasserin |4 aut | |
| 700 | 1 | |a Wiedeking, M. |e verfasserin |4 aut | |
| 700 | 1 | |a Sieja, K. |e verfasserin |4 aut | |
| 700 | 1 | |a Bleuel, D. L. |e verfasserin |4 aut | |
| 700 | 1 | |a Brits, C. P. |e verfasserin |4 aut | |
| 700 | 1 | |a Bucher, T. D. |e verfasserin |4 aut | |
| 700 | 1 | |a Dinoko, T. S. |e verfasserin |4 aut | |
| 700 | 1 | |a Easton, J. L. |e verfasserin |4 aut | |
| 700 | 1 | |a Görgen, A. |e verfasserin |4 aut | |
| 700 | 1 | |a Guttormsen, M. |e verfasserin |4 aut | |
| 700 | 1 | |a Jones, P. |e verfasserin |4 aut | |
| 700 | 1 | |a Kheswa, B. V. |e verfasserin |4 aut | |
| 700 | 1 | |a Khumalo, N. A. |e verfasserin |4 aut | |
| 700 | 1 | |a Larsen, A. C. |e verfasserin |4 aut | |
| 700 | 1 | |a Lawrie, E. A. |e verfasserin |4 aut | |
| 700 | 1 | |a Lawrie, J. J. |e verfasserin |4 aut | |
| 700 | 1 | |a Majola, S. N. T. |e verfasserin |4 aut | |
| 700 | 1 | |a Malatji, K. L. |e verfasserin |4 aut | |
| 700 | 1 | |a Makhathini, L. |e verfasserin |4 aut | |
| 700 | 1 | |a Maqabuka, B. |e verfasserin |4 aut | |
| 700 | 1 | |a Negi, D. |e verfasserin |4 aut | |
| 700 | 1 | |a Noncolela, S. P. |e verfasserin |4 aut | |
| 700 | 1 | |a Papka, P. |e verfasserin |4 aut | |
| 700 | 1 | |a Sahin, E. |e verfasserin |4 aut | |
| 700 | 1 | |a Schwengner, R. |e verfasserin |4 aut | |
| 700 | 1 | |a Tveten, G. M. |e verfasserin |4 aut | |
| 700 | 1 | |a Zeiser, F. |e verfasserin |4 aut | |
| 700 | 1 | |a Zikhali, B. R. |e verfasserin |4 aut | |
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10.1140/epja/s10050-020-00070-7 doi (DE-627)SPR008300747 (SPR)s10050-020-00070-7-e DE-627 ger DE-627 rakwb eng 530 ASE 33.40 bkl 33.50 bkl Ingeberg, V. W. verfasserin aut First application of the Oslo method in inverse kinematics 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The %$\gamma %$-ray strength function (%$\gamma %$SF) and nuclear level density (NLD) have been extracted for the first time from inverse kinematic reactions with the Oslo method. This novel technique allows measurements of these properties across a wide range of previously inaccessible nuclei. Proton–%$\gamma %$ coincidence events from the %$\mathrm {d}(^{86}\mathrm {Kr}, \mathrm {p}\gamma )^{87}\mathrm {Kr}%$ reaction were measured at iThemba LABS and the %$\gamma %$SF and NLD in %$^{87}\mathrm {Kr}%$ was obtained. The low-energy region of the %$\gamma %$SF is compared to shell-model calculations, which suggest this region to be dominated by M1 strength. The %$\gamma %$SF and NLD are used as input parameters to Hauser–Feshbach calculations to constrain %$(\mathrm {n},\gamma )%$ cross sections of nuclei using the TALYS reaction code. These results are compared to %$^{86}\mathrm {Kr}(n,\gamma )%$ data from direct measurements. Siem, S. verfasserin aut Wiedeking, M. verfasserin aut Sieja, K. verfasserin aut Bleuel, D. L. verfasserin aut Brits, C. P. verfasserin aut Bucher, T. D. verfasserin aut Dinoko, T. S. verfasserin aut Easton, J. L. verfasserin aut Görgen, A. verfasserin aut Guttormsen, M. verfasserin aut Jones, P. verfasserin aut Kheswa, B. V. verfasserin aut Khumalo, N. A. verfasserin aut Larsen, A. C. verfasserin aut Lawrie, E. A. verfasserin aut Lawrie, J. J. verfasserin aut Majola, S. N. T. verfasserin aut Malatji, K. L. verfasserin aut Makhathini, L. verfasserin aut Maqabuka, B. verfasserin aut Negi, D. verfasserin aut Noncolela, S. P. verfasserin aut Papka, P. verfasserin aut Sahin, E. verfasserin aut Schwengner, R. verfasserin aut Tveten, G. M. verfasserin aut Zeiser, F. verfasserin aut Zikhali, B. R. verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 56(2020), 2 vom: 20. Feb. (DE-627)25372290X (DE-600)1459066-9 1434-601X nnns volume:56 year:2020 number:2 day:20 month:02 https://dx.doi.org/10.1140/epja/s10050-020-00070-7 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.40 ASE 33.50 ASE AR 56 2020 2 20 02 |
| spelling |
10.1140/epja/s10050-020-00070-7 doi (DE-627)SPR008300747 (SPR)s10050-020-00070-7-e DE-627 ger DE-627 rakwb eng 530 ASE 33.40 bkl 33.50 bkl Ingeberg, V. W. verfasserin aut First application of the Oslo method in inverse kinematics 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The %$\gamma %$-ray strength function (%$\gamma %$SF) and nuclear level density (NLD) have been extracted for the first time from inverse kinematic reactions with the Oslo method. This novel technique allows measurements of these properties across a wide range of previously inaccessible nuclei. Proton–%$\gamma %$ coincidence events from the %$\mathrm {d}(^{86}\mathrm {Kr}, \mathrm {p}\gamma )^{87}\mathrm {Kr}%$ reaction were measured at iThemba LABS and the %$\gamma %$SF and NLD in %$^{87}\mathrm {Kr}%$ was obtained. The low-energy region of the %$\gamma %$SF is compared to shell-model calculations, which suggest this region to be dominated by M1 strength. The %$\gamma %$SF and NLD are used as input parameters to Hauser–Feshbach calculations to constrain %$(\mathrm {n},\gamma )%$ cross sections of nuclei using the TALYS reaction code. These results are compared to %$^{86}\mathrm {Kr}(n,\gamma )%$ data from direct measurements. Siem, S. verfasserin aut Wiedeking, M. verfasserin aut Sieja, K. verfasserin aut Bleuel, D. L. verfasserin aut Brits, C. P. verfasserin aut Bucher, T. D. verfasserin aut Dinoko, T. S. verfasserin aut Easton, J. L. verfasserin aut Görgen, A. verfasserin aut Guttormsen, M. verfasserin aut Jones, P. verfasserin aut Kheswa, B. V. verfasserin aut Khumalo, N. A. verfasserin aut Larsen, A. C. verfasserin aut Lawrie, E. A. verfasserin aut Lawrie, J. J. verfasserin aut Majola, S. N. T. verfasserin aut Malatji, K. L. verfasserin aut Makhathini, L. verfasserin aut Maqabuka, B. verfasserin aut Negi, D. verfasserin aut Noncolela, S. P. verfasserin aut Papka, P. verfasserin aut Sahin, E. verfasserin aut Schwengner, R. verfasserin aut Tveten, G. M. verfasserin aut Zeiser, F. verfasserin aut Zikhali, B. R. verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 56(2020), 2 vom: 20. Feb. (DE-627)25372290X (DE-600)1459066-9 1434-601X nnns volume:56 year:2020 number:2 day:20 month:02 https://dx.doi.org/10.1140/epja/s10050-020-00070-7 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.40 ASE 33.50 ASE AR 56 2020 2 20 02 |
| allfields_unstemmed |
10.1140/epja/s10050-020-00070-7 doi (DE-627)SPR008300747 (SPR)s10050-020-00070-7-e DE-627 ger DE-627 rakwb eng 530 ASE 33.40 bkl 33.50 bkl Ingeberg, V. W. verfasserin aut First application of the Oslo method in inverse kinematics 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The %$\gamma %$-ray strength function (%$\gamma %$SF) and nuclear level density (NLD) have been extracted for the first time from inverse kinematic reactions with the Oslo method. This novel technique allows measurements of these properties across a wide range of previously inaccessible nuclei. Proton–%$\gamma %$ coincidence events from the %$\mathrm {d}(^{86}\mathrm {Kr}, \mathrm {p}\gamma )^{87}\mathrm {Kr}%$ reaction were measured at iThemba LABS and the %$\gamma %$SF and NLD in %$^{87}\mathrm {Kr}%$ was obtained. The low-energy region of the %$\gamma %$SF is compared to shell-model calculations, which suggest this region to be dominated by M1 strength. The %$\gamma %$SF and NLD are used as input parameters to Hauser–Feshbach calculations to constrain %$(\mathrm {n},\gamma )%$ cross sections of nuclei using the TALYS reaction code. These results are compared to %$^{86}\mathrm {Kr}(n,\gamma )%$ data from direct measurements. Siem, S. verfasserin aut Wiedeking, M. verfasserin aut Sieja, K. verfasserin aut Bleuel, D. L. verfasserin aut Brits, C. P. verfasserin aut Bucher, T. D. verfasserin aut Dinoko, T. S. verfasserin aut Easton, J. L. verfasserin aut Görgen, A. verfasserin aut Guttormsen, M. verfasserin aut Jones, P. verfasserin aut Kheswa, B. V. verfasserin aut Khumalo, N. A. verfasserin aut Larsen, A. C. verfasserin aut Lawrie, E. A. verfasserin aut Lawrie, J. J. verfasserin aut Majola, S. N. T. verfasserin aut Malatji, K. L. verfasserin aut Makhathini, L. verfasserin aut Maqabuka, B. verfasserin aut Negi, D. verfasserin aut Noncolela, S. P. verfasserin aut Papka, P. verfasserin aut Sahin, E. verfasserin aut Schwengner, R. verfasserin aut Tveten, G. M. verfasserin aut Zeiser, F. verfasserin aut Zikhali, B. R. verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 56(2020), 2 vom: 20. Feb. (DE-627)25372290X (DE-600)1459066-9 1434-601X nnns volume:56 year:2020 number:2 day:20 month:02 https://dx.doi.org/10.1140/epja/s10050-020-00070-7 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.40 ASE 33.50 ASE AR 56 2020 2 20 02 |
| allfieldsGer |
10.1140/epja/s10050-020-00070-7 doi (DE-627)SPR008300747 (SPR)s10050-020-00070-7-e DE-627 ger DE-627 rakwb eng 530 ASE 33.40 bkl 33.50 bkl Ingeberg, V. W. verfasserin aut First application of the Oslo method in inverse kinematics 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The %$\gamma %$-ray strength function (%$\gamma %$SF) and nuclear level density (NLD) have been extracted for the first time from inverse kinematic reactions with the Oslo method. This novel technique allows measurements of these properties across a wide range of previously inaccessible nuclei. Proton–%$\gamma %$ coincidence events from the %$\mathrm {d}(^{86}\mathrm {Kr}, \mathrm {p}\gamma )^{87}\mathrm {Kr}%$ reaction were measured at iThemba LABS and the %$\gamma %$SF and NLD in %$^{87}\mathrm {Kr}%$ was obtained. The low-energy region of the %$\gamma %$SF is compared to shell-model calculations, which suggest this region to be dominated by M1 strength. The %$\gamma %$SF and NLD are used as input parameters to Hauser–Feshbach calculations to constrain %$(\mathrm {n},\gamma )%$ cross sections of nuclei using the TALYS reaction code. These results are compared to %$^{86}\mathrm {Kr}(n,\gamma )%$ data from direct measurements. Siem, S. verfasserin aut Wiedeking, M. verfasserin aut Sieja, K. verfasserin aut Bleuel, D. L. verfasserin aut Brits, C. P. verfasserin aut Bucher, T. D. verfasserin aut Dinoko, T. S. verfasserin aut Easton, J. L. verfasserin aut Görgen, A. verfasserin aut Guttormsen, M. verfasserin aut Jones, P. verfasserin aut Kheswa, B. V. verfasserin aut Khumalo, N. A. verfasserin aut Larsen, A. C. verfasserin aut Lawrie, E. A. verfasserin aut Lawrie, J. J. verfasserin aut Majola, S. N. T. verfasserin aut Malatji, K. L. verfasserin aut Makhathini, L. verfasserin aut Maqabuka, B. verfasserin aut Negi, D. verfasserin aut Noncolela, S. P. verfasserin aut Papka, P. verfasserin aut Sahin, E. verfasserin aut Schwengner, R. verfasserin aut Tveten, G. M. verfasserin aut Zeiser, F. verfasserin aut Zikhali, B. R. verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 56(2020), 2 vom: 20. Feb. (DE-627)25372290X (DE-600)1459066-9 1434-601X nnns volume:56 year:2020 number:2 day:20 month:02 https://dx.doi.org/10.1140/epja/s10050-020-00070-7 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.40 ASE 33.50 ASE AR 56 2020 2 20 02 |
| allfieldsSound |
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Ingeberg, V. W. @@aut@@ Siem, S. @@aut@@ Wiedeking, M. @@aut@@ Sieja, K. @@aut@@ Bleuel, D. L. @@aut@@ Brits, C. P. @@aut@@ Bucher, T. D. @@aut@@ Dinoko, T. S. @@aut@@ Easton, J. L. @@aut@@ Görgen, A. @@aut@@ Guttormsen, M. @@aut@@ Jones, P. @@aut@@ Kheswa, B. V. @@aut@@ Khumalo, N. A. @@aut@@ Larsen, A. C. @@aut@@ Lawrie, E. A. @@aut@@ Lawrie, J. J. @@aut@@ Majola, S. N. T. @@aut@@ Malatji, K. L. @@aut@@ Makhathini, L. @@aut@@ Maqabuka, B. @@aut@@ Negi, D. @@aut@@ Noncolela, S. P. @@aut@@ Papka, P. @@aut@@ Sahin, E. @@aut@@ Schwengner, R. @@aut@@ Tveten, G. M. @@aut@@ Zeiser, F. @@aut@@ Zikhali, B. R. @@aut@@ |
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| author |
Ingeberg, V. W. |
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Ingeberg, V. W. ddc 530 bkl 33.40 bkl 33.50 First application of the Oslo method in inverse kinematics |
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530 - Physics |
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530 ASE 33.40 bkl 33.50 bkl First application of the Oslo method in inverse kinematics |
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ddc 530 bkl 33.40 bkl 33.50 |
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ddc 530 bkl 33.40 bkl 33.50 |
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Elektronische Aufsätze Aufsätze Elektronische Ressource |
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The European physical journal |
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First application of the Oslo method in inverse kinematics |
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First application of the Oslo method in inverse kinematics |
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Ingeberg, V. W. |
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The European physical journal |
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The European physical journal |
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eng |
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2020 |
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Ingeberg, V. W. Siem, S. Wiedeking, M. Sieja, K. Bleuel, D. L. Brits, C. P. Bucher, T. D. Dinoko, T. S. Easton, J. L. Görgen, A. Guttormsen, M. Jones, P. Kheswa, B. V. Khumalo, N. A. Larsen, A. C. Lawrie, E. A. Lawrie, J. J. Majola, S. N. T. Malatji, K. L. Makhathini, L. Maqabuka, B. Negi, D. Noncolela, S. P. Papka, P. Sahin, E. Schwengner, R. Tveten, G. M. Zeiser, F. Zikhali, B. R. |
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530 ASE 33.40 bkl 33.50 bkl |
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Elektronische Aufsätze |
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Ingeberg, V. W. |
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10.1140/epja/s10050-020-00070-7 |
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530 |
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verfasserin |
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first application of the oslo method in inverse kinematics |
| title_auth |
First application of the Oslo method in inverse kinematics |
| abstract |
Abstract The %$\gamma %$-ray strength function (%$\gamma %$SF) and nuclear level density (NLD) have been extracted for the first time from inverse kinematic reactions with the Oslo method. This novel technique allows measurements of these properties across a wide range of previously inaccessible nuclei. Proton–%$\gamma %$ coincidence events from the %$\mathrm {d}(^{86}\mathrm {Kr}, \mathrm {p}\gamma )^{87}\mathrm {Kr}%$ reaction were measured at iThemba LABS and the %$\gamma %$SF and NLD in %$^{87}\mathrm {Kr}%$ was obtained. The low-energy region of the %$\gamma %$SF is compared to shell-model calculations, which suggest this region to be dominated by M1 strength. The %$\gamma %$SF and NLD are used as input parameters to Hauser–Feshbach calculations to constrain %$(\mathrm {n},\gamma )%$ cross sections of nuclei using the TALYS reaction code. These results are compared to %$^{86}\mathrm {Kr}(n,\gamma )%$ data from direct measurements. |
| abstractGer |
Abstract The %$\gamma %$-ray strength function (%$\gamma %$SF) and nuclear level density (NLD) have been extracted for the first time from inverse kinematic reactions with the Oslo method. This novel technique allows measurements of these properties across a wide range of previously inaccessible nuclei. Proton–%$\gamma %$ coincidence events from the %$\mathrm {d}(^{86}\mathrm {Kr}, \mathrm {p}\gamma )^{87}\mathrm {Kr}%$ reaction were measured at iThemba LABS and the %$\gamma %$SF and NLD in %$^{87}\mathrm {Kr}%$ was obtained. The low-energy region of the %$\gamma %$SF is compared to shell-model calculations, which suggest this region to be dominated by M1 strength. The %$\gamma %$SF and NLD are used as input parameters to Hauser–Feshbach calculations to constrain %$(\mathrm {n},\gamma )%$ cross sections of nuclei using the TALYS reaction code. These results are compared to %$^{86}\mathrm {Kr}(n,\gamma )%$ data from direct measurements. |
| abstract_unstemmed |
Abstract The %$\gamma %$-ray strength function (%$\gamma %$SF) and nuclear level density (NLD) have been extracted for the first time from inverse kinematic reactions with the Oslo method. This novel technique allows measurements of these properties across a wide range of previously inaccessible nuclei. Proton–%$\gamma %$ coincidence events from the %$\mathrm {d}(^{86}\mathrm {Kr}, \mathrm {p}\gamma )^{87}\mathrm {Kr}%$ reaction were measured at iThemba LABS and the %$\gamma %$SF and NLD in %$^{87}\mathrm {Kr}%$ was obtained. The low-energy region of the %$\gamma %$SF is compared to shell-model calculations, which suggest this region to be dominated by M1 strength. The %$\gamma %$SF and NLD are used as input parameters to Hauser–Feshbach calculations to constrain %$(\mathrm {n},\gamma )%$ cross sections of nuclei using the TALYS reaction code. These results are compared to %$^{86}\mathrm {Kr}(n,\gamma )%$ data from direct measurements. |
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| title_short |
First application of the Oslo method in inverse kinematics |
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https://dx.doi.org/10.1140/epja/s10050-020-00070-7 |
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| author2 |
Siem, S. Wiedeking, M. Sieja, K. Bleuel, D. L. Brits, C. P. Bucher, T. D. Dinoko, T. S. Easton, J. L. Görgen, A. Guttormsen, M. Jones, P. Kheswa, B. V. Khumalo, N. A. Larsen, A. C. Lawrie, E. A. Lawrie, J. J. Majola, S. N. T. Malatji, K. L. Makhathini, L. Maqabuka, B. Negi, D. Noncolela, S. P. Papka, P. Sahin, E. Schwengner, R. Tveten, G. M. Zeiser, F. Zikhali, B. R. |
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Siem, S. Wiedeking, M. Sieja, K. Bleuel, D. L. Brits, C. P. Bucher, T. D. Dinoko, T. S. Easton, J. L. Görgen, A. Guttormsen, M. Jones, P. Kheswa, B. V. Khumalo, N. A. Larsen, A. C. Lawrie, E. A. Lawrie, J. J. Majola, S. N. T. Malatji, K. L. Makhathini, L. Maqabuka, B. Negi, D. Noncolela, S. P. Papka, P. Sahin, E. Schwengner, R. Tveten, G. M. Zeiser, F. Zikhali, B. R. |
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10.1140/epja/s10050-020-00070-7 |
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2024-07-03T18:31:19.770Z |
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|
| score |
7.401991 |